Ex situ spectroscopic ellipsometry investigation of the layered structure of polycrystalline diamond thin films grown by electron cyclotron resonance-assisted chemical vapor deposition

Citation
S. Gupta et al., Ex situ spectroscopic ellipsometry investigation of the layered structure of polycrystalline diamond thin films grown by electron cyclotron resonance-assisted chemical vapor deposition, J APPL PHYS, 90(3), 2001, pp. 1280-1285
Citations number
29
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
JOURNAL OF APPLIED PHYSICS
ISSN journal
00218979 → ACNP
Volume
90
Issue
3
Year of publication
2001
Pages
1280 - 1285
Database
ISI
SICI code
0021-8979(20010801)90:3<1280:ESSEIO>2.0.ZU;2-#
Abstract
Polycrystalline diamond thin films deposited by electron cyclotron resonanc e-assisted chemical vapor deposition on Si (111) were investigated using sp ectroscopic phase-modulated ellipsometry from the near IR to UV range (830- 270 nm). Analysis of the raw ellipsometry data [psi(lambda (i)), Delta(lamb da (i))] by applying the conventional Bruggeman effective medium theory and linear regression analysis provided details about the film microstructure: (i) the multilayer structure and the component layer thickness of the film s; (ii) the volume fraction of the constituents (sp(3)- and sp(2)- bonded c arbon) and of voids (f(v)) in the bulk layer (L-2); (iii) the inhomogeneity of the structure along the growth axis and its variation with the seeding density; and (iv) the surface roughness layer thickness (d(S)). A simplifie d three-layer structural model consisting of an interfacial layer, an inter mediate (or bulk) layer, and a top surface roughness layer has been propose d that simulates the ellipsometry data reasonably well. The results obtaine d through ellipsometry modeling, such as surface roughness and overall film thickness, were compared with those from atomic force microscopy and profi lometry, respectively, in order to validate the model employed. Typically, high surface roughness values around 60 nm were found for films grown under different substrate temperatures and oxygen-to-carbon ratios. It was also found that a combination of relatively high substrate temperature and O/C r atio can be used to reduce the surface roughness to around 25 nm. In genera l, the void fraction (f(v)) of the bulk layer decreases as a function of se eding density, indicating the formation of a denser film. The sp(2)-bonded carbon fraction (f(sp)(C)(2)) also varies with the process parameters. Thes e results (f(v) and f(sp)(2) (C)) for the bulk layer and its behavior with respect to process parameters are discussed. (C) 2001 American Institute of Physics.